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Exactly Energy Conserving Semi-Implicit Particle in Cell Formulation

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arxiv 1602.06326 v2 pith:FF3QTDY6 submitted 2016-02-18 physics.comp-ph physics.plasm-ph

classification physics.comp-phphysics.plasm-ph
keywords computationalenergymethodsemi-implicittimeexactlyexplicitparticle
verification ladder T0 review T1 audit T2 compute T3 formal
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We report a new particle in cell (PIC) method based on the semi-implicit approach. The novelty of the new method is that unlike any of its semi-implicit predecessors at the same time retains the explicit computational cycle and conserves energy exactly. Recent research has presented fully implicit methods where energy conservation is obtained as part of a non linear iteration procedure. The new method (referred to as Energy Conserving Semi-Implicit Method, ECSIM), instead, does not require any non-linear iteration and its computational cycle is similar to that of explicit PIC. The properties of the new method are: i) it conserves energy exactly to round-off for any time step or grid spacing; ii) it is unconditionally stable in time, freeing the user from the need to resolve the electron plasma frequency and allowing the user to select any desired time step; iii) it eliminates the constraint of the finite grid instability, allowing the user to select any desired resolution without being forced to resolve the Debye length; iv) the particle mover has a computational complexity identical to that of the explicit PIC, only the field solver has an increased computational cost. The new ECSIM is tested in a number of benchmarks where accuracy and computational performance are tested.

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Cited by 1 Pith paper

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Suppressing spurious oscillations and particle noise in particle-in-cell simulations

    physics.comp-ph 2025-06 conditional novelty 6.0 of 10

    The authors suppress spurious oscillations and particle noise in semi-implicit PIC by adding limited Lax-Friedrichs diffusion to the Maxwell solver and computing current in the plasma's moving frame.

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